00:02
Magnetic fields, so you get the magnitude of the magnetic field of a long straight wire using amper's law.
00:11
And this gives us the relationship that the magnetic field strength is equal to the permeability of free space, mu not, times the current i, divided by 2 pi times the distance.
00:32
Between the observation point and the wire.
00:35
So this is for a long wire.
00:40
To get the direction of the magnetic field, you would use the right -hand rule, placing your thumb along the current, and your fingers make circles around the wire in the direction of the magnetic field.
00:56
But the other thing to realize is that if you have multiple wires or multiple sources of magnetic field, you simply add up the individual contributions from each of the sources.
01:11
And magnetic field is a vector, so you need to be a little bit careful about directions.
01:17
The other thing about long wires is that they do exert a magnetic force, well, magnetic field will exert a force on a long wire in the amount il, l being the direction of current flow along the wire, and the magnitude of l being the length crossed into the magnetic field.
01:44
So as an example of this, we have two wires each carrying the same current, we'll call them wire one and wire two, and we will orient the top wire carrying the current to the right, bottom wire carrying current to the left.
02:04
And there are a couple of points that we want to find.
02:07
The total magnetic field at a and b.
02:12
And then we will find the force they exert on each other.
02:18
So that's kind of the process, but it would be good if we use the right -hand rule.
02:24
And for the top wire, what we have is its magnetic field is coming out of the board at the top and going in at the bottom.
02:35
And of course, there's a wrap -around, a certain, around that.
02:41
The bottom wire, it's the opposite, so it goes in on the top, two goes into the board, on top of the wire, and out of the board on the bottom.
02:58
And again, we have a circulation around the wire of those magnetic fields.
03:06
So at a, what we can see is at point a, the magnetic fields add together they are both into the page and so we would add the strength of both of them together to get the full strength and we know the distance and the current in each wire equal distance and that r is 0 .0075 meters and multiply by two because they each have the same strength at that point being midway.
04:00
Now the permability of free space is 4 pi times 10 to the minus seventh in the si units.
04:10
The current is 2 .5 amps.
04:14
That is an si unit, so perfectly good to include 2 .5 amps, and then multiply by 2, divide by 2 pi.
04:28
Yes, that usually works with the top and divide by 7 .5 millimeters will give us the total magnetic field strength in terms of tesla's.
04:59
And that will give us 1 .33 times 10 to the minus 4 tesla.
05:11
Looking at observation point b, what we have is b1.
05:16
The further wire is going into the page.
05:22
B1 goes into the page and it is weaker.
05:28
B2 is coming out of the page, and it is stronger because it is closer...